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  2. Topology of (1D) Quantum Systems Out of Equilibrium

    www.tcm.phy.cam.ac.uk/~nrc25/SEMINARS/topology_ooe_vilnius-used.pdf
    2 Aug 2018: Chern number can be obtained by tomography of Bloch statesTwo-band model: |uk (t)〉 = sin(θk/2)|A, k〉 cos(θk/2) exp(iφk )|B, k〉. ... N. Fläschner, B. S. Rem, M. Tarnowski,. D. Vogel, D.-S. Lühmann, K.
  3. 1 Nov 2018: CA =. 0. B@cos sin 0sin cos 0. 0 0 1. ... X cos Y sin. Again, U () must act on X this way if it is indeed to correspond to arotation.
  4. lectV4.dvi

    www.damtp.cam.ac.uk/user/ms100/LECTURES/lectV4.pdf
    13 Dec 2018: A cosB sin nθ n 6= 0(2.22). Returning to (2.18),. ... Hence, we obtain possible solutions to (2.17) as. Φ = RΘ =. . (C D ln r)(A Bθ) n = 0. (Crn Drn)(A cosB sin nθ) n 6=
  5. lectV4_temp.dvi

    www.damtp.cam.ac.uk/user/ms100/LECTURES/tensors.pdf
    13 Dec 2018: Example: if a and b are vectors then a. b is a scalar. ... b/|a| |b| = cos θ is a scalar, so that the angle between vectors is unaffected by a changeof frame.
  6. GroupsOscar Randal-Williams…

    https://www.dpmms.cam.ac.uk/~or257/teaching/notes/groups.pdf
    28 Nov 2018: A group (G, ,e) is abelian2 if for all a,b G we have a b = b a. ... f ′(f(z)) =a′(azbczd) b. ′. c′(azbczd) d′. =a′(az b) b′(cz d).
  7. Answers.dvi

    https://www.dpmms.cam.ac.uk/~twk10/Answers.pdf
    8 Jan 2018: 53. K43. Observe that. f(h) f(0)h. = |hsinh4| |h| 0. as h 0.If x 6= 0, then f ′(x) = 2xsinx4 4x2 cos x4. ... K87. Very similar to K86. To obtain the formula for un, observe that2 cos2 φ = 1 cos 2φ and cos(π/4) = 21/2.
  8. Intégration et MesureCours de Emmanuel GrenierNotes de Alexis…

    https://www.dpmms.cam.ac.uk/~aptm3/docs/lecture-notes/L3-Integration-Mesure.pdf
    29 Apr 2018: Ceci prouve que A A, A Y σ(L). De même, B B, X B σ(L). ... Il suffit de prouver que 1I Vect (en, n Z).On écrit I = [ch,c h] et on pose :. ϕ : t [a,b] 7 12 [cos (ω(t c)) cos(ωh)].
  9. ijrr

    mi.eng.cam.ac.uk/~cipolla/publications/article/1997-IJRR-divergence-deformation-report.pdf
    13 Mar 2018: divv = (ux vy) (3). curlv = (uy vx) (4). (defv) cos 2µ = (ux vy) (5). ... Z0(56). curlv = 23 (qU1 pU2). Z0(57). (defv) cos 2µ =(pU1 qU2).
  10. bmvc08.dvi

    mi.eng.cam.ac.uk/~cipolla/publications/inproceedings/2008-BMVC-gesture-interface.pdf
    13 Mar 2018: Input. v2. u2. θ2. Online Update. P1. P2. Manifold Learning. θΣby cos i. ... b) the low-dimensional manifoldrepresentation allows matching that is both time and memoryefficient.
  11. ijrr

    mi.eng.cam.ac.uk/~cipolla/archive/Publications/article/1997-IJRR-divergence-deformation-report.pdf
    13 Mar 2018: divv = (ux vy) (3). curlv = (uy vx) (4). (defv) cos 2µ = (ux vy) (5). ... Z0(56). curlv = 23 (qU1 pU2). Z0(57). (defv) cos 2µ =(pU1 qU2).
  12. bmvc08.dvi

    mi.eng.cam.ac.uk/~cipolla/archive/Publications/inproceedings/2008-BMVC-gesture-interface.pdf
    13 Mar 2018: Input. v2. u2. θ2. Online Update. P1. P2. Manifold Learning. θΣby cos i. ... b) the low-dimensional manifoldrepresentation allows matching that is both time and memoryefficient.
  13. Vortices, Painlevé integrability andprojective geometry Felipe…

    www.damtp.cam.ac.uk/user/md327/felipe_thesis.pdf
    3 Apr 2018: 1/C0 sin(. C0κ1) cos κ3φ2. /C0 sin(. C0κ1) sin κ3φ1. ]J2 cos(. ... Aκ1 = φ2J1 φ1J2. Aκ2 =1C0. sin(C0κ1)φ1J1. 1C0. sin(C0κ1)φ2J2+. cos(C0κ1)J3. A direct calculation shows that this gauge potential is indeed GC0-equivariant.
  14. École Normale Supérieure de LyonResearch internship report Geometry…

    https://www.dpmms.cam.ac.uk/~aptm3/docs/maths/2018-GeometryCoxeterGroups-Abridged.pdf
    17 Aug 2018: cos(0) = 1).We then define B to be the symmetric bilinear form on V = RS whose matrix in the canonicalbasis (es)sS is C. ... Y ) ((t,y) , (t′,y′))2 = t2 t′2 2tt′ cos (min{π,dY (y,y′)}).
  15. M. Pettini: Introduction to Cosmology — Lecture 16 DARK ...

    https://people.ast.cam.ac.uk/~pettini/Intro%20Cosmology/Lecture16.pdf
    22 Nov 2018: systemic velocity of the galaxyindicated by the Doppler shift of the nucleus, and b/a = cos i is the ratioof the minor to the major axis of the ellipse that a ... Right : The observer sees distorted, correlated, images of the distant galaxies.The
  16. Epipolar geometry from profiles under circular motion - Pattern…

    mi.eng.cam.ac.uk/~cipolla/publications/article/2001-PAMI-circular-motion.pdf
    13 Mar 2018: S 1cosÿ. ÿcos ÿ2 sin cos 2d cos ÿ2 sin cos cos 2d sin. ... transformation is further reduced to a bilateral symmetry,. given by. B ÿcos 2 ÿsin 2 2d cos ÿsin 2 cos 2 2d sin.
  17. IEEE TRANSACTIONS ON PATTERN ANALYSIS AND MACHINE INTELLIGENCE, VOL.…

    mi.eng.cam.ac.uk/~cipolla/publications/article/2003-PAMI-Wong.pdf
    13 Mar 2018: 0 0 cos(φ θ).  , (14). wheredl = u0 cos θ v0 sin θ. ... will then become abilateral symmetry, given by. B =. . cos 2θ sin 2θ 2dl cos θ sin 2θ cos 2θ 2dl sin θ.
  18. GROUPS SIMON WADSLEY Contents 1. Examples of groups 21.1. ...

    https://www.dpmms.cam.ac.uk/~sjw47/LecturesM17.pdf
    16 Nov 2018: ThenAzz̄ Bz̄ B̄z C = 0 |z B/A|2 = |B|2/A2 C/A. ... For z C, z = f(z) if and onlyif cz2 dz az b = 0.
  19. Epipolar geometry from profiles under circular motion - Pattern…

    mi.eng.cam.ac.uk/~cipolla/archive/Publications/article/2001-PAMI-circular-motion.pdf
    13 Mar 2018: S 1cosÿ. ÿcos ÿ2 sin cos 2d cos ÿ2 sin cos cos 2d sin. ... transformation is further reduced to a bilateral symmetry,. given by. B ÿcos 2 ÿsin 2 2d cos ÿsin 2 cos 2 2d sin.
  20. MNRAS 000, 1–21 (2017) Preprint 14 June 2018 Compiled ...

    https://people.ast.cam.ac.uk/~wyatt/wvkb17.pdf
    14 Jun 2018: transit,. tcross(b = 0) =(. 2R?G M? ) rt/(1+ e cos $). ... rt < 0.31(1+ e cos $) (22). in au, and so rt < 0.62 au.
  21. ProSHADE: src/proshade/ProSHADE_clipper.cpp Source File

    https://www2.mrc-lmb.cam.ac.uk/groups/murshudov/content/proshade/doxygen/d9/d66/_pro_s_h_a_d_e__clipper_8cpp_source.html
    1 Nov 2018: 122 //======================================== Find axis ranges & change B-factors if required.
  22. IEEE TRANSACTIONS ON PATTERN ANALYSIS AND MACHINE INTELLIGENCE, VOL.…

    mi.eng.cam.ac.uk/~cipolla/archive/Publications/article/2003-PAMI-Wong.pdf
    13 Mar 2018: 0 0 cos(φ θ).  , (14). wheredl = u0 cos θ v0 sin θ. ... will then become abilateral symmetry, given by. B =. . cos 2θ sin 2θ 2dl cos θ sin 2θ cos 2θ 2dl sin θ.
  23. Structured Deep Neural Networks for Speech Recognition

    mi.eng.cam.ac.uk/~mjfg/thesis_cw564.pdf
    12 Jul 2018: regularisations on sigmoid stimulated DNNs. 1135.6 WSJ-SI84: Comparison of activation grid outputs of raw, KL, Cos and. ... That is, suppose a simple linear function is applied2:. φ(z) = W Tz b.
  24. KL843-03.tex

    mi.eng.cam.ac.uk/~cipolla/publications/article/1999-IJCV-generalised-epipolar.pdf
    13 Mar 2018: 1B = cos(b1) sin(b1) b2sin(b1) cos(b1) b3. 0 0 1.  ,1C =.  c1 cos(c2) c1 sin(c2) c3c1 sin(c2) c1 cos(c2) c40 0 ... Figure 7. Rectification of uncalibrated images. (a) and (b): Thefigures show two images.
  25. KL843-03.tex

    mi.eng.cam.ac.uk/~cipolla/archive/Publications/article/1999-IJCV-generalised-epipolar.pdf
    13 Mar 2018: 1B = cos(b1) sin(b1) b2sin(b1) cos(b1) b3. 0 0 1.  ,1C =.  c1 cos(c2) c1 sin(c2) c3c1 sin(c2) c1 cos(c2) c40 0 ... Figure 7. Rectification of uncalibrated images. (a) and (b): Thefigures show two images.

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